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CN111177641B - Wire temperature rise assessment method under high wind speed - Google Patents

Wire temperature rise assessment method under high wind speed Download PDF

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Publication number
CN111177641B
CN111177641B CN201911336407.0A CN201911336407A CN111177641B CN 111177641 B CN111177641 B CN 111177641B CN 201911336407 A CN201911336407 A CN 201911336407A CN 111177641 B CN111177641 B CN 111177641B
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wire
temperature
temperature rise
average value
wind speed
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CN111177641A (en
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赵新宇
贾振宏
张瑞永
姚成
奚海波
袁飞
郭瑞兴
缪旭瑞
陈剑
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China Energy Engineering Group Jiangsu Power Design Institute Co Ltd
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    • G06COMPUTING; CALCULATING OR COUNTING
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Abstract

The invention discloses a wire temperature rise assessment method under high wind speed, which comprises the steps of obtaining the temperature T on the circumference of the cross section of each wire to be tested and calculating the average value of the temperature T
Figure DDA0002331045930000011
Calculating the temperature T and the average value
Figure DDA0002331045930000012
Is the average value of the sum of absolute values of the differences of (a)
Figure DDA0002331045930000013
According to the average value
Figure DDA0002331045930000014
The condition of (1) realizes the temperature rise evaluation of the lead; the method can calculate or experiment the uneven increase of the temperature distribution of the lifting wire at a high wind speed, judge the uneven increase of the temperature of the wire, then determine the maximum allowable current-carrying capacity of the wire by improving the calculation precision, and has important engineering value for excavating the potential power transmission capacity of the existing power grid.

Description

Wire temperature rise assessment method under high wind speed
Technical Field
The invention belongs to the field of power transmission and transformation, and particularly relates to a wire temperature rise assessment method under high wind speed.
Background
With the improvement of the power transmission voltage level (1000 kV alternating current and 1100kV direct current), the mode of improving the power transmission capacity by improving the power transmission voltage level is extremely used by human beings, and with the development of computational disciplines, the scholars of each country re-study the heat load capacity of the wire, and the maximum allowable current-carrying capacity of the wire is determined by improving the computational accuracy, so that the method has important engineering value for mining the potential power transmission capacity of the existing power grid. With the rapid increase of the wire temperature distribution nonuniformity in the calculation or experiment of the wind speed, how to judge the nonuniformity of the wire temperature rise is lacking in a corresponding method at present.
Disclosure of Invention
In order to solve the technical problems in the prior art, the invention provides a wire temperature rise assessment method under high wind speed.
The invention solves the technical problems by the following technical proposal:
the wire temperature rise assessment method under high wind speed comprises the following steps:
s1, acquiring the temperature T on the circumference of the cross section of each wire to be tested;
s2, calculating the average value of the temperatures T on the circumferences of the cross sections of all the wires to be tested obtained in the step S1
Figure BDA0002331045910000011
S3, calculating the temperature T on the circumference of the cross section of each wire to be tested obtained in the step S1 and the average value obtained in the step S2
Figure BDA0002331045910000012
Absolute value of the difference of (2)Average value of the sum of values ∈ ->
Figure BDA0002331045910000019
S4, obtaining an average value according to the step S3
Figure BDA00023310459100000110
The condition of (2) realizes the wire temperature rise assessment.
Further, in the step S1, the temperature T on the circumference of the cross section of each wire to be measured is obtained by using an optical fiber temperature measurement method.
Further, in the step S2, an average value
Figure BDA0002331045910000015
The calculation formula of (2) is as follows:
Figure BDA0002331045910000016
the integration is performed along the arc of the cross section of the wire to be measured, and dl is the differential value of the arc of the cross section of the wire to be measured.
Further, in the step S3, an average value
Figure BDA00023310459100000111
The calculation formula of (2) is as follows:
Figure BDA0002331045910000018
further, in the step S4, when
Figure BDA00023310459100000210
When the temperature rise of the wire is estimated, the lee side of the wire to be measured is selected by the measuring point; when->
Figure BDA00023310459100000211
And when the temperature rise of the wire is estimated, the measuring point can be selected to be any position on the surface of the wire to be measured.
Preferably, the wire to be tested is an overhead bare wire.
The beneficial effects of the invention are as follows:
according to the invention, based on the thermal load capacity technology of the wire, the temperature distribution non-uniformity of the wire is increased sharply along with the calculation or experiment of the temperature distribution non-uniformity of the wire at a high wind speed, the non-uniformity of the temperature rise of the wire is judged, and then the maximum allowable current-carrying capacity of the wire is determined by improving the calculation precision, so that the method has important engineering value for excavating the potential power transmission capacity of the existing power grid.
Drawings
Fig. 1 is a flow chart of the present invention.
Fig. 2 is a cross-sectional view of a wire under test of the present invention.
Detailed Description
For the purpose of making the objects, technical solutions and advantages of the embodiments of the present invention more apparent, the technical solutions of the embodiments of the present invention will be clearly and completely described below with reference to the accompanying drawings in the embodiments of the present invention, and it is apparent that the described embodiments are some embodiments of the present invention, but not all embodiments of the present invention. The components of the embodiments of the present invention generally described and illustrated in the figures herein may be arranged and designed in a wide variety of different configurations.
Examples
As shown in fig. 1, a method for evaluating temperature rise of a wire under high wind speed includes the following steps:
s1, acquiring the temperature T on the circumference of each wire cross section to be measured, wherein the wire cross section to be measured is shown in FIG. 2;
s2, calculating the average value of the temperatures T on the circumferences of the cross sections of all the wires to be tested obtained in the step S1
Figure BDA0002331045910000023
S3, calculating the temperature T on the circumference of the cross section of each wire to be tested obtained in the step S1 and the average value obtained in the step S2
Figure BDA0002331045910000024
Absolute value of the difference between (a) and (b)Average value of sum->
Figure BDA00023310459100000212
S4, obtaining an average value according to the step S3
Figure BDA00023310459100000213
The condition of (2) realizes the wire temperature rise assessment.
In this embodiment, in step S1, the temperature T on the circumference of the cross section of each wire to be measured is obtained by using an optical fiber temperature measurement method.
In this embodiment, in the step S2, the average value
Figure BDA0002331045910000027
The calculation formula of (2) is as follows:
Figure BDA0002331045910000028
the integration is performed along the arc of the cross section of the wire to be measured, and dl is the differential value of the arc of the cross section of the wire to be measured.
In this embodiment, in the step S3, the average value
Figure BDA00023310459100000214
The calculation formula of (2) is as follows:
Figure BDA0002331045910000031
in this embodiment, in the step S4, when
Figure BDA0002331045910000034
When the temperature rise of the wire is estimated, the lee side of the wire to be measured is selected by the measuring point; when->
Figure BDA0002331045910000035
And when the temperature rise of the wire is estimated, the measuring point can be selected to be any position on the surface of the wire to be measured.
In this embodiment, the to-be-tested wire is an overhead bare wire.
The foregoing is merely a preferred embodiment of the present invention and it should be noted that modifications and adaptations to those skilled in the art may be made without departing from the principles of the present invention, which are intended to be comprehended within the scope of the present invention.

Claims (4)

1. A wire temperature rise assessment method under high wind speed is characterized in that: the method comprises the following steps:
s1, acquiring the temperature T on the circumference of the cross section of each wire to be tested;
s2, calculating the average value of the temperatures T on the circumferences of the cross sections of all the wires to be tested obtained in the step S1
Figure FDA0004242176520000011
S3, calculating the temperature T on the circumference of the cross section of each wire to be tested obtained in the step S1 and the average value obtained in the step S2
Figure FDA0004242176520000012
Average value of the sum of absolute values of the differences +.>
Figure FDA0004242176520000013
S4, obtaining an average value according to the step S3
Figure FDA0004242176520000014
The condition of (1) realizes the temperature rise evaluation of the lead;
in the step S2, the average value
Figure FDA0004242176520000015
The calculation formula of (2) is as follows:
Figure FDA0004242176520000016
the integration is carried out along the arc of the cross section of the wire to be measured, and dl is the differential value of the arc of the cross section of the wire to be measured;
in the step S4, when
Figure FDA0004242176520000017
When the temperature rise of the wire is estimated, the lee side of the wire to be measured is selected by the measuring point; when (when)
Figure FDA0004242176520000018
And when the temperature rise of the wire is estimated, the measuring point can be selected to be any position on the surface of the wire to be measured.
2. The method for evaluating the temperature rise of a wire at a high wind speed according to claim 1, wherein the method comprises the following steps: in the step S1, the temperature T on the circumference of the cross section of each wire to be measured is obtained by using an optical fiber temperature measurement method.
3. The method for evaluating the temperature rise of a wire at a high wind speed according to claim 1, wherein the method comprises the following steps: in the step S3, the average value
Figure FDA0004242176520000019
The calculation formula of (2) is as follows:
Figure FDA00042421765200000110
4. the method for evaluating the temperature rise of a wire under high wind speed according to claim 1, wherein the wire to be tested is an overhead bare wire.
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Citations (4)

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Publication number Priority date Publication date Assignee Title
GB1542916A (en) * 1975-12-03 1979-03-28 Achenbach Buschhuetten Gmbh Method and apparatus for controlling the flatness of strip material
RU2189019C2 (en) * 2000-11-29 2002-09-10 Научно-исследовательский центр прикладной электродинамики Казанского государственного технического университета им. А.Н.Туполева Method of contactless measurements of average volume temperature of object made from dielectric material
CN109766659A (en) * 2019-01-28 2019-05-17 重庆科技学院 A kind of conductor sag calculation method for considering wind load and conduction time and influencing
CN109973332A (en) * 2017-12-27 2019-07-05 浙江中自庆安新能源技术有限公司 Blade of wind-driven generator icing on-line monitoring method and device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5742861B2 (en) * 2013-02-28 2015-07-01 横河電機株式会社 Optical fiber temperature distribution measuring device

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1542916A (en) * 1975-12-03 1979-03-28 Achenbach Buschhuetten Gmbh Method and apparatus for controlling the flatness of strip material
RU2189019C2 (en) * 2000-11-29 2002-09-10 Научно-исследовательский центр прикладной электродинамики Казанского государственного технического университета им. А.Н.Туполева Method of contactless measurements of average volume temperature of object made from dielectric material
CN109973332A (en) * 2017-12-27 2019-07-05 浙江中自庆安新能源技术有限公司 Blade of wind-driven generator icing on-line monitoring method and device
CN109766659A (en) * 2019-01-28 2019-05-17 重庆科技学院 A kind of conductor sag calculation method for considering wind load and conduction time and influencing

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
周象贤 ; 温典 ; 王少华 ; 刘岩 ; 蒋愉宽 ; 李特 ; .高压架空输电线路分裂导线温度场仿真分析.电工电气.2017,(03),全文. *
朱永灿 ; 黄新波 ; 贾建援 ; 程丹 ; 林淑凡 ; 张烨 ; .输电线路覆冰导线对流换热的数值模拟.高电压技术.2015,(10),全文. *
胡剑 等.基于热网络模型的架空输电线路径向和周向温度计算方法.《电工技术学报》.2019,34(1),第139-152页. *
高强 ; 陈希 ; 侯继勇 ; 仝杰 ; 雷煜卿 ; .OPPC表面温度场与流场的数值模拟研究.电力系统通信.2013,(02),全文. *

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